TW201209930A - Generation of multiple diameter nanowire field effect transistors - Google Patents

Generation of multiple diameter nanowire field effect transistors Download PDF

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Publication number
TW201209930A
TW201209930A TW100116198A TW100116198A TW201209930A TW 201209930 A TW201209930 A TW 201209930A TW 100116198 A TW100116198 A TW 100116198A TW 100116198 A TW100116198 A TW 100116198A TW 201209930 A TW201209930 A TW 201209930A
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Taiwan
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nanowire
semiconductor
region
channel
channels
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TW100116198A
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Chinese (zh)
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TWI512836B (en
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Sarunya Bangsaruntip
Guy M Cohen
Jeffrey W Sleight
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Ibm
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
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    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/0657Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape of the body
    • H01L29/0665Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape of the body the shape of the body defining a nanostructure
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    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/04Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their crystalline structure, e.g. polycrystalline, cubic or particular orientation of crystalline planes
    • H01L29/045Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their crystalline structure, e.g. polycrystalline, cubic or particular orientation of crystalline planes by their particular orientation of crystalline planes
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y10/00Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y30/00Nanotechnology for materials or surface science, e.g. nanocomposites
    • BPERFORMING OPERATIONS; TRANSPORTING
    • B82NANOTECHNOLOGY
    • B82YSPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
    • B82Y40/00Manufacture or treatment of nanostructures
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    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/30Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
    • H01L21/302Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to change their surface-physical characteristics or shape, e.g. etching, polishing, cutting
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    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
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    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/30Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
    • H01L21/324Thermal treatment for modifying the properties of semiconductor bodies, e.g. annealing, sintering
    • H01L21/3247Thermal treatment for modifying the properties of semiconductor bodies, e.g. annealing, sintering for altering the shape, e.g. smoothing the surface
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    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/06Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions
    • H01L29/0657Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape of the body
    • H01L29/0665Semiconductor bodies ; Multistep manufacturing processes therefor characterised by their shape; characterised by the shapes, relative sizes, or dispositions of the semiconductor regions ; characterised by the concentration or distribution of impurities within semiconductor regions characterised by the shape of the body the shape of the body defining a nanostructure
    • H01L29/0669Nanowires or nanotubes
    • H01L29/0673Nanowires or nanotubes oriented parallel to a substrate
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    • H01L29/40Electrodes ; Multistep manufacturing processes therefor
    • H01L29/41Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions
    • H01L29/423Electrodes ; Multistep manufacturing processes therefor characterised by their shape, relative sizes or dispositions not carrying the current to be rectified, amplified or switched
    • H01L29/42312Gate electrodes for field effect devices
    • H01L29/42316Gate electrodes for field effect devices for field-effect transistors
    • H01L29/4232Gate electrodes for field effect devices for field-effect transistors with insulated gate
    • H01L29/42384Gate electrodes for field effect devices for field-effect transistors with insulated gate for thin film field effect transistors, e.g. characterised by the thickness or the shape of the insulator or the dimensions, the shape or the lay-out of the conductor
    • H01L29/42392Gate electrodes for field effect devices for field-effect transistors with insulated gate for thin film field effect transistors, e.g. characterised by the thickness or the shape of the insulator or the dimensions, the shape or the lay-out of the conductor fully surrounding the channel, e.g. gate-all-around
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    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/66007Multistep manufacturing processes
    • H01L29/66075Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials
    • H01L29/66227Multistep manufacturing processes of devices having semiconductor bodies comprising group 14 or group 13/15 materials the devices being controllable only by the electric current supplied or the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched, e.g. three-terminal devices
    • H01L29/66409Unipolar field-effect transistors
    • H01L29/66439Unipolar field-effect transistors with a one- or zero-dimensional channel, e.g. quantum wire FET, in-plane gate transistor [IPG], single electron transistor [SET], striped channel transistor, Coulomb blockade transistor
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    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/775Field effect transistors with one dimensional charge carrier gas channel, e.g. quantum wire FET
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    • H01L29/66Types of semiconductor device ; Multistep manufacturing processes therefor
    • H01L29/68Types of semiconductor device ; Multistep manufacturing processes therefor controllable by only the electric current supplied, or only the electric potential applied, to an electrode which does not carry the current to be rectified, amplified or switched
    • H01L29/76Unipolar devices, e.g. field effect transistors
    • H01L29/772Field effect transistors
    • H01L29/78Field effect transistors with field effect produced by an insulated gate
    • H01L29/786Thin film transistors, i.e. transistors with a channel being at least partly a thin film
    • H01L29/78696Thin film transistors, i.e. transistors with a channel being at least partly a thin film characterised by the structure of the channel, e.g. multichannel, transverse or longitudinal shape, length or width, doping structure, or the overlap or alignment between the channel and the gate, the source or the drain, or the contacting structure of the channel

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  • Engineering & Computer Science (AREA)
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  • Crystallography & Structural Chemistry (AREA)
  • Manufacturing & Machinery (AREA)
  • Materials Engineering (AREA)
  • Mathematical Physics (AREA)
  • Theoretical Computer Science (AREA)
  • Composite Materials (AREA)
  • Thin Film Transistor (AREA)

Abstract

A method of modifying a wafer having a semiconductor disposed on an insulator is provided and includes forming first and second nanowire channels connected at each end to semiconductor pads at first and second wafer regions, respectively, with second nanowire channel sidewalls being misaligned relative to a crystallographic plane of the semiconductor more than first nanowire channel sidewalls and displacing the semiconductor toward an alignment condition between the sidewalls and the crystallographic plane such that thickness differences between the first and second nanowire channels reflect the greater misalignment of the second nanowire channel sidewalls.

Description

201209930 六、發明說明: 【發明所屬之技術領域】 本發明之態樣係針對生產多重直徑之奈米線場效電晶 體(field effect transistors; FETs)之方法。 【先前技術】 作為未來互補金氧半導體(CMOS)部件設計之選擇,奈 米線FET正在引起人們相當大的關注。雖然正在取得進 展,但仍待考慮若干關鍵問題。在此等問題中,一個特 定問題為將要求奈米線F E T元件提供具有不同驅動電流 強度及/或不同閾電壓(Vt)之元件。 <似屯风5虫度及/或不 同閾電壓之元件的問題之解決辦法,但該等解決辦法通 常依賴於藉由相應調變閘極工作函數() 來調變元件之間電壓。因此’此等解決辦法傾向於具有 相對困難且成本高昂之製程整合操作並且,另外,該等 解決辦法傾向於呈現變更關係。 κ 【發明内容】 根據本發明之—態樣,本發明提供—種方法,兮方法 =有安置於一絕緣體上之—半導體之-晶圓,該方 ^下步驟:形成各末端分別連接至處於第-及第 201209930 二晶圓區域之半導體襯墊之第一及第二奈米線通道,而 第二奈米線通道側壁較第一奈米線通道側壁相對於該半 導體之一結晶面(crystallographic plane )更為錯位 (misaligned );以及自該等第一及第二奈米線通道向其 該等側壁與該結晶面之間的一對準條件位移半導體材 料’以使得該位移之後該等第一及第二奈米線通道之間 的厚度差異反映該第二奈求線通道側壁之該較大的錯 位。 根據本發明之一態樣,本發明提供一種修改具有安置 於—絕緣體上之一半導體之一晶圓的方法,該方法包括 以下步驟:形成各末端分別連接至處於第一及第二晶圓 區域之半導體襯墊之第一及第二奈米線通道,而第一奈 米線通道側壁以相對於該半導體之一結晶面之一第一對 準度特徵化’而第二奈米線通道以相對於該結晶面之一 第二對準度特徵化,該第二對準度不同於該第一對準 度;以及促使(encourage )半導體材料自該等第一及第 一奈米線通道向該等側壁與該結晶面之間的一對準條件 位移,以使得該位移之後在該等第一及第二奈米線通道 之間的厚度差異與該第一及第二對準度差異一致。 根據本發明之一態樣,本發明提供一種修改具有安置 於-絕緣體上之-半導體之一晶圓,該方法包括以下步 驟··在該晶圓之一第一區域中形成由奈米線通道連接之 半導體襯墊對,該等奈米線通道具有沿該半導體之(110) 結晶面定向之其長軸及大體上平行於該半導體之該等 201209930 {110}面中之一者之側壁;在該晶圓之—第二區域中形成 由奈米線通道連接之半導體襯墊對,該等奈米線通道具 有相對於該半導體之該等{i 10}結晶面成一角度之其長 軸及同樣相對於該半導體之該等{110}面成一角度之側 壁;以及再定向該第二區域之該等奈米線通道,以藉由 將半導體材料自該等奈米線通道擴散至該等襯墊形成平 行於該半導體之該等{丨丨0 }面之側壁,以使得該第二區域 中之該專奈米線通道與處於該第一區域之彼等奈米線通 道相比受到薄化(thinned )。 根據本發明之另一態樣,本發明提供一種晶圓,該晶 圓包括一基板、安置於該基板上之一埋藏氧化物(buried oxide; BOX)層及安置於該BOX層上之第一及第二區域 處之一絕緣體上覆石夕(silicon-on-insulator; SOI)結構,在 各區域處之該S 01結構具有經由其中形成之各個奈米線 通道連接之各個SOI襯墊對,處於該等區域中之一者之 該等SOI襯墊及該等奈米線通道較處於該等區域中之另 一者之該等SOI襯墊及該等奈米線通道相對於該so〗之 {110}面更為錯位。 【實施方式】 本文經由關於矽(Si)奈米線及Si處理之描述提供支撑 例如環繞閘極(gate-all-around; GAA)奈米線場效電晶體 (FETs)之結構以及用於製造該等電晶體之方法。然而, 6 201209930 本技術亦可由諸如例如鍺(Ge)之其他半導體材料實施。 田使用含# Sl I導體時,纟教示之處理步驟類似於且適 合於所用之特定半導體。因此’諸如Si、妙錯(siGe)、 Si/SiGe、碳化矽(Sic)或碳化矽鍺(siGeC)之含&半導體 材料之使用僅理解為示例性的。 參看第1圖及第2圖’提供晶圓i,且其包括Si基板 ιοί、埋藏氧化物(Β〇χ)層1〇2及絕緣體上覆矽層 W3。晶圓1可使用諸如注氧隔離(Separati〇n时 IMplanted 〇Xygen; SIM〇x)或晶圓黏合(例如 SmartCut )之方法製造。此等晶圓製造技術為熟習此項 技術者已知,因此本文不再進一步描述。亦可以本領域 所已知之其他SOI基板取代本文所述之Β〇χ構造上之 SOI’且其將在本教示之範喻之内。 曰曰圓1至少具有建立於其上之一第一區域1〇及一第二 區域20。801襯墊(103~對及將其連接之奈米線通道1〇4 可被圊案化至處於第一區域1〇及第二區域2〇之s〇I層 1 〇3中,以在各區域中形成例如梯狀結構。奈米線通道 及SOI襯墊103A之圖案化可經由微影技術(例如光 束戈電子束)及隨後的活性離子Ί4刻(reactive ion etching’ RIE)或經由側壁移置技術達成。此等圖案化技 術為熟習此項技術者已知。 處於第一區域1〇及第二區域2〇之s〇I層1〇3最初各 自由具有相似厚度之相似元件形成。然而,如第丨圖及 第2圖所不’處於第一區域之s〇I襯墊i〇3A及奈米 201209930 線通道104經形成具有大體上平行於及/或對準於例如 半導體之{110}結晶面中之一者的側壁,然而其他平面參 考坐標系是可能的《亦即,奈米線通道丨04中之每一者 之主(長)軸沿半導體之{ i i 〇 }結晶面之方向定向。另一 方面’處於第二區域20之SOI襯墊103A及奈米線通道 104經形成具有相對於{11〇丨結晶面成角度α及/或以角 度α錯位之側壁’其中奈米線通道1 〇4之主(長)軸亦 相對於{110}結晶面以角度α錯位.。舉例而言,第一區域 10中之奈米線通道1 〇4可經圊案化以具有平行於丨丨丨〇) 面之側壁及平行於{1〇〇}面之頂面,而第二區域2〇中之 奈米線通道104將具有相對於{丨丨〇)結晶面以角度α (諸 如α=1度)錯位之側壁及平行於{1〇〇}面之頂面。 在第二區域20之奈米線通道104成角度及/或錯位之 情況下,如上所述’對第一區域10及第二區域兩者 進行的薄化操作(例如奈米線通道丨〇4之退火)將傾向 於在第一區域20處比在第一區域1〇具有更大的薄化效 應。此狀況由於處於第二區域2〇之S0I層ι〇3之偏位 L aa取向使處於第二區域20之SOI層103比第一區域 10之SOI層103對薄化操作之效應更為敏感。該薄化操 作傾向於再定向第二區域2〇之奈米線通道1〇4,以藉由 將半導體材料自奈米線通道104擴散至s〇I襯墊1〇3A 形成平行於{ 1 1 〇 }結晶面之側壁。此舉具有第二區域2 Q 中之奈米線通道104在再定向之後比第一區域1〇之彼等 通道變得更薄之效應。 201209930 4 -區域20之SOI層1〇3被薄化超過第一區域⑺ 之S〇I|103之程度可藉由增加或減少第一區域1〇及 第:區域20之側壁之相對錯位來控制。舉例而言,處於 第-區域10之奈米線通道1Q4之側壁可相對於該半導體 之{110}結晶面對準,或僅以一小角度α錯位。同時,處 於第一區域20之奈米線通道1〇4之側壁可相對於該半導 體之(no)結晶面以一較大角度α.#意錯位。此處,第一 區域10及第二區域20之側壁之相對錯位越大,則在該 第二區域20處之薄化程度越大。 確實,參看第2圖,奈米線通道104相對於{11〇}結晶 面之角度α可為小於45。之任何角度(且實務上α不超 過幾度)’條件為該角度之傾斜越大,則所得再成形奈米 線108將越薄。亦即,成更傾斜角度之奈米線通道1〇4 將比更垂直之奈米線通道104傾向於形成更薄之再成形 奈米線108。因此’儘管奈米線通道丨〇4之尺寸及其傾 斜度可根據設計考慮而變化’但奈米線通道1 之輪廓 (profile )應涵蓋所要形成之再成形奈米線丨〇8之至少 一輪廓。 其中石夕自奈米線通道104擴散之再定向處理在g.M.201209930 VI. Description of the Invention: [Technical Field of the Invention] The aspect of the present invention is directed to a method of producing multi-diameter nanowire field effect transistors (FETs). [Prior Art] As a choice of future complementary metal oxide semiconductor (CMOS) component designs, nanowire FETs are attracting considerable attention. Although progress is being made, a number of key issues remain to be considered. Among these problems, a particular problem is that the nanowire F E T component will be required to provide components having different drive current intensities and/or different threshold voltages (Vt). <Solutions for problems with components such as hurricane 5 worms and/or different threshold voltages, but such solutions typically rely on modulating the voltage between components by a corresponding modulating gate function (). Therefore, these solutions tend to have relatively difficult and costly process integration operations and, in addition, these solutions tend to present a change relationship. κ [Abstract] According to the invention, the present invention provides a method, a method of arranging a semiconductor-wafer disposed on an insulator, and the following steps: forming the ends to be respectively connected to The first and second nanowire channels of the semiconductor pads of the second and second layers of the 201209930, and the sidewalls of the second nanowire channel are opposite to the crystallographic plane of the semiconductor of the first nanowire channel (crystallographic The plane is more misaligned; and the semiconductor material is displaced from the first and second nanowire channels to an alignment condition between the sidewalls and the crystal face such that the displacement is after the The difference in thickness between the first and second nanowire channels reflects the larger misalignment of the sidewalls of the second nanowire channel. According to an aspect of the present invention, there is provided a method of modifying a wafer having a semiconductor disposed on an insulator, the method comprising the steps of: forming respective ends to be respectively connected to the first and second wafer regions First and second nanowire channels of the semiconductor pad, and the sidewalls of the first nanowire channel are characterized by a first alignment with respect to one of the crystal faces of the semiconductor; and the second nanowire channel is Characterizing the second alignment relative to one of the crystal faces, the second alignment being different from the first alignment; and encuring the semiconductor material from the first and first nanowire channels An alignment condition between the sidewalls and the crystallized surface is such that a difference in thickness between the first and second nanowire channels after the displacement is consistent with the first and second alignment degrees . According to an aspect of the present invention, there is provided a method of modifying a wafer having a semiconductor disposed on an insulator, the method comprising the steps of: forming a nanowire channel connection in a first region of the wafer a pair of semiconductor pads having a major axis oriented along a (110) crystal plane of the semiconductor and a sidewall substantially parallel to one of the 201209930 {110} faces of the semiconductor; Forming, in the second region of the wafer, a pair of semiconductor pads connected by a nanowire channel having a major axis at an angle relative to the {i 10} crystal faces of the semiconductor and the same relative Forming an angled sidewall on the {110} faces of the semiconductor; and reorienting the nanowire channels of the second region to form a semiconductor material from the nanowire channels to the pads Parallel to the sidewalls of the {丨丨0 } faces of the semiconductor such that the antenna line channels in the second region are thinned compared to the nanowire channels in the first region (thinned ). According to another aspect of the present invention, the present invention provides a wafer including a substrate, a buried oxide (BOX) layer disposed on the substrate, and a first layer disposed on the BOX layer And a silicon-on-insulator (SOI) structure at one of the second regions, the S 01 structures at each region having respective SOI pad pairs connected via respective nanowire channels formed therein, The SOI pads and the nanowire channels in one of the regions are opposite to the SOI pads and the nanowire channels of the other of the regions The {110} face is more misplaced. [Embodiment] Provided herein are structures for supporting, for example, gate-all-around (GAA) nanowire field effect transistors (FETs) and for fabrication via the description of germanium (Si) nanowires and Si processing. The method of the transistor. However, 6 201209930 the present technology can also be implemented by other semiconductor materials such as, for example, germanium (Ge). When the field uses a #Sl I conductor, the processing steps are similar and suitable for the particular semiconductor used. Therefore, the use of <semiconductor materials such as Si, SiGe, Si/SiGe, Sic or SiGeC is understood to be merely exemplary. The wafer i is provided with reference to Figs. 1 and 2, and includes a Si substrate ιοί, a buried oxide (Β〇χ) layer 1〇2, and an insulator overlying layer W3. Wafer 1 can be fabricated using methods such as oxygen injection isolation (IMplanted® Xygen; SIM〇x) or wafer bonding (eg, SmartCut). Such wafer fabrication techniques are known to those skilled in the art and are therefore not further described herein. Other SOI substrates known in the art may also be substituted for the SOI's described herein and which are within the teachings of the present teachings. The dome 1 has at least one of the first region 1〇 and the second region 20. The 801 pad (the 103~ pair and the nanowire channel 1〇4 connected thereto can be patterned to be in The first region 1 〇 and the second region 2 〇 〇 I layer 1 〇 3 to form, for example, a ladder structure in each region. The patterning of the nanowire channel and the SOI liner 103A can be via lithography ( For example, a beam of electron beams) and subsequent reactive ion etching (RIE) or via sidewall displacement techniques. Such patterning techniques are known to those skilled in the art. The two regions 2 〇 〇 I layer 1 〇 3 are initially formed by similar elements having similar thicknesses. However, as shown in the first and second figures, the s〇I pad i 〇 3A in the first region and Nano 201209930 line channel 104 is formed to have sidewalls that are substantially parallel to and/or aligned to one of the {110} crystal faces of, for example, a semiconductor, although other planar reference coordinate systems are possible, ie, nanowires The main (long) axis of each of the channels 丨04 is along the { ii 〇} crystal plane of the semiconductor Directional orientation. On the other hand, the SOI liner 103A and the nanowire channel 104 in the second region 20 are formed to have a side wall with an angle α with respect to the {11〇丨 crystal plane and/or with an angle α. The main (long) axis of the line channel 1 〇4 is also offset by an angle α with respect to the {110} crystal plane. For example, the nanowire channel 1 〇4 in the first region 10 can be patterned to have parallel The side wall of the face is parallel to the top surface of the {1〇〇} face, and the nanowire channel 104 in the second zone 2〇 will have an angle α with respect to the {丨丨〇) crystal face ( The side wall of the misalignment such as α = 1 degree and the top surface of the {1〇〇} plane. In the case where the nanowire channel 104 of the second region 20 is angled and/or misaligned, as described above, the thinning operation is performed on both the first region 10 and the second region (for example, the nanowire channel 丨〇4) The annealing) will tend to have a greater thinning effect at the first region 20 than at the first region 1〇. This condition is more sensitive to the effect of the thinning operation of the SOI layer 103 in the second region 20 than the SOI layer 103 in the first region 10 due to the offset of the SOI layer ι3 in the second region. The thinning operation tends to redirect the second region 2N of the nanowire channel 1〇4 to form a parallel to {1 1 by diffusing the semiconductor material from the nanowire channel 104 to the s〇I pad 1〇3A. 〇}The side wall of the crystal face. This has the effect that the nanowire channels 104 in the second region 2 Q become thinner after the reorientation than the channels of the first region 1〇. 201209930 4 - The degree to which SOI layer 1〇3 of region 20 is thinned beyond S〇I|103 of first region (7) can be controlled by increasing or decreasing the relative misalignment of the sidewalls of first region 1 and region 20 . For example, the sidewalls of the nanowire channel 1Q4 at the first region 10 may be aligned with respect to the {110} crystal plane of the semiconductor, or may be misaligned only by a small angle a. At the same time, the side wall of the nanowire channel 1〇4 of the first region 20 may be offset by a larger angle α.# with respect to the (no) crystal plane of the semiconductor. Here, the greater the relative misalignment of the sidewalls of the first region 10 and the second region 20, the greater the degree of thinning at the second region 20. Indeed, referring to Fig. 2, the angle α of the nanowire channel 104 relative to the {11〇} crystal plane may be less than 45. Any angle (and practically α does not exceed a few degrees)' condition is that the greater the slope of the angle, the thinner the resulting reshaped nanowire 108 will be. That is, the nanowire channel 1〇4 at a more oblique angle tends to form a thinner reshaped nanowire 108 than the more vertical nanowire channel 104. Therefore 'although the size and inclination of the nanowire channel 丨〇4 can vary depending on design considerations', the profile of the nanowire channel 1 should cover at least one of the reshaped nanowires 8 to be formed. profile. Among them, Shi Xi’s re-orientation treatment from the diffusion of the channel 104 in g.M.

Cohen 等人之來自 San Francisco, CA (2010)之 Material Research Symposium 的「Controlling the shape and dimensional variability of top-down fabricated silicon nanowires by hydrogen annealing」中有更充分之描述, 其内容以引用之方式併入本文。晶面方向之規格遵循密 201209930 勒指數(Miller indices)規定’其在例如杨㈣^及 Mennin之固態物理學(1976)之第5章中有所描述,其内 容以引用之方式併入本文。遵循此規定,一晶面族(亦 即根據晶體之對稱性等效之平面)通常藉由—對{}括號 引用。舉例而言’面(_、㈣)及⑽υ在—立方結晶 中全部等效。-者以{10〇}面代表其全體。當引用結晶t 之方向時,使用[]方括弧,例如[100]、[〇1〇]、[〇〇1]、 [-100]、[0-10]、[0(M],且同樣地,以<1〇〇>代表一結晶 方向族全體。 因此’處於第二區域20之奈米線通道1〇4可經形成成 為再成形奈米線108(見第3圖)’再成形奈米線1〇8較 第-區域10之彼等奈米線更薄,即使其中在各區域處以 類似方式進行退火處理。詳言之,第一區域1〇之再成形 奈米線H)8將具有厚度Τι,,且第4域2q之再成形奈 米線108將具有厚度T2.,厚度T2.將不同於厚度Tl.且通 常較厚度TV更薄。因此,在第一區域1〇及第二區域2〇 處之再成形奈米線1〇8之此等相對厚度差異將導致再成 形奈米線108顯示可彼此獨特之物理特性。 奈米線通道104之成角度可以不同方式實現。舉例而 言,微影技術遮罩可包括對於區域1〇及區域2〇之拉拔 狀態(as-drawn)對準圖案及錯位圖案,或在成角度奈 米線通道1G4之㈣化期間,晶圓丨或㈣化遮罩可相 對於(11〇}結晶面旋轉。然而,奈米線通H04之成角度 無須處於任何特定結晶面中’且上述(11(^結晶面僅理解 10 201209930 為示例性的。 參看第3圖’奈米線通道1 〇4成為奈米線1 〇8之再成 形通常藉由在惰性氣氛中退火實現。此處理可為同時或 順序應用於區域10及區域20之無遮罩處理。 例如’晶圓1可在示例性Hz氣氛中退火。在此Η?退 火之前不久’可自奈米線通道1 〇4之側壁及S0I襯塾 1〇3A蝕刻掉原生氧化物。該H2中之退火具有若干目 的’包括但不限於平滑化奈米線通道1 04之側壁、將該 等側壁重新對準至SOI襯墊103A之結晶面、將奈米線 通道1 04橫剖面從矩形再成形為更加圓柱形以及經由si 之再分佈將奈米線通道丨〇4主體薄化。 根據一示例性實施例,該惰性氣體退火在以下條件下 進行.自約3 0托(Torr)至約1000托之氣壓、自約攝 氏600度(°〇至約1100〇c之溫度及長達約1分鐘至約12〇 分鉍之持續時間。大體而言’ S i再分佈速率隨溫度而增 大且隨壓力增大而減小。 如第3圖所示,奈米線通道1〇4可再成形為奈米線 108,且經由該退火處理或經由box層i 〇2之進一步蝕 刻及凹陷而懸置於BOX層102上或自BOX層1〇2釋放。 再成形奈米線108因此在第一區域1〇及第二區域2〇中 之SOI襯墊ι〇3Α之間及凹陷氧化物1〇5上方形成懸置 的橋接件(suspended bridges)。可達成BOX層1〇2之 凹陷’其為由該退火處理所致,或使用稀釋氫氟酸 (diluted hydrofluoric; DHF)蝕刻以底切 BOX 層 1〇2。儘 201209930 管SOI基板提供界定及懸置奈米線通道1〇4及/或再成形 米線108之便利途徑,但有可能由其他基板獲得懸 置。舉例而言’在主體Si晶圓上磊晶生長之㈣^丨堆 疊亦可經圖案化而形成奈米線通冑1〇4及/或再成形奈 米線1 〇8。SiGe層亦可用作被底切之犧牲層(類似於B0X 層 102)。 處於第一區域10且具有厚度TV之再成形奈米線108 及處於第二區域2〇且具有厚度T2,之再成形奈米線ι〇8 可具有不同之驅動電流及/或閾電壓。以此方式,應當瞭 解,可藉由相應地控制部分決定最終厚度Τι,及h,之處 於第一區域ίο及第二區域20之奈米線通道1〇4之成角 度來控制至少處於晶圓1之第-區域10及第二區域20 之電路特性。 見參看第4圖及第5圖,閘極結構4〇2可圍繞再成形 不米線108形成。f先,用第一及第三閉極介電質“Μ 及112 t覆再成形奈米線1〇8。第一(且可任選)閉極 介電質112A通常為Si〇2。第二閘極介電質ιΐ2可包括 氧化矽(Si〇2)、氮氧化矽(Si〇N)、二氧化銓(η⑺2)或任 何其他合適之一或多種高k介電質,且對於§1〇2及si〇N 而。可利用化學氣相沈積(CVD)、原子層沈積(ald)或氧 化爐進行’尤積。然後,可形成例如TaN $㈣之薄閘極 導體1 1 7之保形沈積。此舉之後可為摻雜多晶梦⑴之 沈積,以在環繞再成形奈米,線1〇8之周邊形成閘極堆叠 118。遮罩115可用於促進經由例如RIE触刻閉極線。 12 201209930 • 在閘極堆疊118之外的薄閘極導體117之一部分可經由 RIE移除,或在替代性實施例中,自閘極堆疊外部表面 移除薄閘極導體117可能需要額外濕式蝕刻操作。 多晶鍺或另一合適之組成物可用作多晶矽丨13之替代 物。另外,任何多晶SiGe摻合物(aU〇y)亦可用於替 代多晶石夕113。更進一步,多晶石夕113能夠以多晶形式 沈積或以非晶形式沈積,該非晶形式當曝露於高溫時隨 後轉變成多晶矽。 儘管已結合示例性實施例描述本揭示案,但熟習此項 技術者應理解,在不脫離本揭示案之範疇的情況下,可 進行各種修改,並且其元件可由等同物替代。此外,在 不脫離其基本範疇之情況下,可進行諸多修改以使特定 情況或材料適合於本揭示案之教示。因此,希望本揭示 案不限於作為所預期用於實施本揭示案之最佳方式所揭 示之特定示例性實施例,但本揭示案將包括落入附加申 請專利範圍之範疇内的全部實施例。 【圖式簡單說明】 被視為本發明之標的在本專利說明書結束處之申請專 利範圍中被特別指出且明確主張。本發明之前述及其他 態樣、特徵結構及優點將從以上詳細描述結合隨附圖式 中顯而易見,其中: 第1圖為在第一及第二區域處具有界定於其上之奈米 13 201209930 線通道之第1圖之晶圓的透視圖; 第2圖為第1圊之奈米線通道之尺寸的平面圖; 第3圖為具有界定於其上之再成形奈米線之第丨圖之 晶圓的透視圖; 第4圖為具有閘極結構之再成形奈米線的透視圖;以 及 , 第5圖包括具有不同厚度之奈米線的橫剖面圖。 【主要元件符號說明】 1 晶圓 20 第二區域 102 埋藏氧化物層 103A SOI襯塾 105 氧化物 112 第二閘極介電質 113 多晶碎 117 薄閘極導體 402 閘極結構 ΤΓ 厚度 10 第一區域 101 Si基板 103 絕緣體上覆矽層 104 奈来線通道 108 再成形奈米線 112A 第一閘極介電質 115 遮罩 118 閘極堆疊 α 角度 τ2· 厚度Cohen et al., "Controlling the shape and dimensional variability of top-down fabricated silicon nanowires by hydrogen annealing" from San Francisco, CA (2010), Material Synthesis Symposium, which is incorporated by reference. This article. The specification of the direction of the crystal faces follows the provisions of the 201209930 Miller indices, which are described, for example, in Chapter 5 of Yang (4) and Mennin's Solid State Physics (1976), the contents of which are incorporated herein by reference. Following this rule, a family of crystal faces (i.e., planes equivalent to the symmetry of the crystal) is usually referenced by the pair of {} brackets. For example, the faces (_, (4)) and (10) are all equivalent in the cubic crystal. - The person is represented by {10〇}. When referring to the direction of the crystal t, use the [] square brackets, such as [100], [〇1〇], [〇〇1], [-100], [0-10], [0(M], and the same Ground, <1〇〇> represents a group of crystal orientations. Therefore, the nanowire channel 1〇4 in the second region 20 can be formed into a reshaped nanowire 108 (see Fig. 3). The formed nanowires 1〇8 are thinner than the nanowires of the first region 10, even though annealing is performed in a similar manner at each region. In detail, the first region 1〇 reshaped nanowire H) 8 will have a thickness Τι, and the reshaped nanowire 108 of the fourth domain 2q will have a thickness T2. The thickness T2. will be different from the thickness Tl. and is generally thinner than the thickness TV. Thus, such relative thickness differences in the reshaped nanowires 1〇8 at the first region 1〇 and the second region 2〇 will cause the reshaped nanowires 108 to exhibit physical properties that are unique to each other. The angle of the nanowire channel 104 can be achieved in different ways. For example, the lithography mask may include an as-drawn alignment pattern and a misalignment pattern for the region 1 and region 2, or during the (iv) period of the angled nanowire channel 1G4. The round or (iv) mask can be rotated relative to the (11〇) crystal plane. However, the angle of the nanowire through H04 does not need to be in any particular crystal plane' and the above (11 (^ crystal plane only understands 10 201209930 as an example) Referring to Figure 3, the recrystallization of the nanowire channel 1 〇4 to the nanowire 1 〇8 is usually achieved by annealing in an inert atmosphere. This treatment can be applied to the regions 10 and 20 simultaneously or sequentially. No mask treatment. For example, 'Wafer 1 can be annealed in an exemplary Hz atmosphere. So far before the annealing?', the raw oxide can be etched away from the sidewall of the nanowire channel 1 〇4 and the S0I liner 1〇3A. The annealing in H2 has several purposes including, but not limited to, smoothing the sidewalls of the nanowire channel 104, realigning the sidewalls to the crystal plane of the SOI liner 103A, and the nanowire channel 104 cross section. Reshaping from a rectangle to a more cylindrical shape and redistribution via si The nanowire channel 丨〇4 body is thinned. According to an exemplary embodiment, the inert gas annealing is performed under the following conditions: from about 30 Torr to about 1000 Torr, from about 600 degrees Celsius (°) 〇 to a temperature of about 1100 〇c and a duration of from about 1 minute to about 12 minutes. In general, the rate of 'S i redistribution increases with temperature and decreases with increasing pressure. As shown, the nanowire channel 1〇4 can be reshaped into a nanowire 108 and suspended on the BOX layer 102 or from the BOX layer 1 via the annealing process or further etching and recessing via the box layer i 〇2. 〇2 release. The reshaped nanowire 108 thus forms a suspended bridge between the first region 1〇 and the SOI liner 〇3〇 in the second region 2〇 and over the recessed oxide 1〇5 (suspended bridges) The depression of the BOX layer 1〇2 can be achieved by the annealing treatment, or by diluted hydrofluoric (DHF) etching to undercut the BOX layer 1〇2. The 201209930 tube SOI substrate is provided to define And a convenient way to suspend the nanowire channel 1〇4 and/or reshape the rice noodle 108, but it may be by other The substrate is suspended. For example, the (four) stacking of epitaxial growth on the bulk Si wafer may also be patterned to form a nanowire pass 1胄4 and/or a reshaped nanowire 1〇8. The SiGe layer can also be used as a sacrificial layer for undercutting (similar to the B0X layer 102). The reshaped nanowire 108 having the thickness TV in the first region 10 and the second region 2〇 having a thickness T2, The shaped nanowire ι 8 can have different drive currents and/or threshold voltages. In this way, it should be understood that at least the wafer can be controlled by the corresponding control portion determining the final thickness Τι, and h, which are at the angle of the first region ίο and the second region 20 of the nanowire channel 1〇4. Circuit characteristics of the first-region 10 and the second region 20 of 1. Referring to Figures 4 and 5, the gate structure 4〇2 can be formed around the reshaped non-rice line 108. f First, the first and third closed-cell dielectrics "Μ and 112 t overmolded nanowires 1〇8. The first (and optionally) closed-electrode dielectric 112A is usually Si〇2. The two-gate dielectric ι 2 may include yttrium oxide (Si〇2), yttrium oxynitride (Si〇N), cerium oxide (η(7)2) or any other suitable one or more high-k dielectrics, and for §1 〇2 and si〇N. It can be formed by chemical vapor deposition (CVD), atomic layer deposition (ALD) or an oxidizing furnace. Then, a thin gate conductor such as TaN $(4) can be formed. Shape deposition. This can be followed by deposition of doped polycrystalline dreams (1) to form a gate stack 118 around the perimeter of the reshaped nano, line 1 。 8. The mask 115 can be used to facilitate the closure of the via via RIE 12 201209930 • A portion of the thin gate conductor 117 outside of the gate stack 118 may be removed via RIE, or in an alternative embodiment, removing the thin gate conductor 117 from the outer surface of the gate stack may require additional Wet etching operation. Polycrystalline germanium or another suitable composition can be used as a substitute for polycrystalline germanium 13. In addition, any polycrystalline SiGe doping The material (aU〇y) can also be used in place of the polycrystalline stone 113. Further, the polycrystalline stone 113 can be deposited in a polycrystalline form or in an amorphous form which is subsequently converted to polycrystalline germanium when exposed to high temperatures. Although the present disclosure has been described in connection with the exemplary embodiments, those skilled in the art should understand that various modifications may be made and the elements may be replaced by equivalents without departing from the scope of the disclosure. Numerous modifications may be made to adapt a particular situation or material to the teachings of the present disclosure. It is therefore contemplated that the disclosure is not limited to the preferred embodiments disclosed. Specific exemplary embodiments, but the disclosure will include all embodiments falling within the scope of the appended claims. [Brief Description] The subject matter of the present invention is considered to be the subject matter of the present application. The foregoing and other aspects, features, and advantages of the present invention will be It is obvious that: Figure 1 is a perspective view of the wafer of Figure 1 with the nanometer 13 201209930 line channel defined on the first and second regions; Figure 2 is the first nanometer. A plan view of the dimensions of the line channel; Figure 3 is a perspective view of the wafer having the second figure of the reshaped nanowire defined thereon; and Figure 4 is a perspective view of the reshaped nanowire with the gate structure And, Fig. 5 includes a cross-sectional view of a nanowire having different thicknesses. [Main component symbol description] 1 Wafer 20 Second region 102 Buried oxide layer 103A SOI lining 105 Oxide 112 Second gate dielectric Electrical 113 Polycrystalline 117 Thin Gate Conductor 402 Gate Structure 厚度 Thickness 10 First Area 101 Si Substrate 103 Insulator Overlying Layer 104 Nea Line Channel 108 Reshaped Nanowire 112A First Gate Dielectric 115 Mask 118 gate stack α angle τ2· thickness

S 14S 14

Claims (1)

201209930 七、申請專利範圍: 1 · 一種修改具有安置於—絕緣體上之一半導體之—晶圓之 方法,該方法包含以下步驟: 形成各末端分別連接至處於第一及第二晶圓區域之 半導體襯墊之第一及第二奈米線通道,而第二奈米線通 道側壁較第一奈米線通道側壁相對於該半導體之一結晶 面在更大程度上錯位(misaligned);以及 自》玄荨第一及第二奈米線通道向其側壁與該結晶面 之間的一對準條件位移半導體材料,以使得該位移之後 該等第一及第二奈米線通道之間的厚度差異反映該等第 二奈米線通道側壁之該較大的錯位。 2. 一種修改具有安置於一絕緣體上之一半導體之一晶圓之 方法,該方法包含以下步驟: 在该晶圓之一第一區域中形成由奈米線通道連接之 半導體概塾對’该等奈米線通道具有沿該半導體之該等 {110}結晶面定向之其長軸,以及大體上平行於該半導體 之該等{ 11 0 }面中之一者之側壁; 在》玄曰曰圓之一第二區域中形成由奈米線通遒連接之 半導體概塾對’該等奈米線通道具有相對於該半導體之 該等{110}結晶面成一角度之其長軸,以及同樣相對於該 半導體之该等{11 〇}面成角度之側壁;以及 再定向該第二區域之該等奈米線通道,以藉由將半 15 201209930 導體材料自該等奈米線通道擴散至該等襯塾形成平行於 該半導體之該等{ 1 1 〇 }面之側壁,以使得該第二區域中之 該等奈米線通道與處於該第一區域之彼等奈米線通道相 比被薄化。 3.如請求項1或請求項2所述之方法,其中該形成之步驟 包含以下步驟:形成彼此平行之該第一區域之該等奈米 線通道,以及形成彼此平行之該第二區域之該等奈米線 通道。 4.如請求項1或請求項2所述之方法,其中該等第一奈米 線通道側壁相對於該結晶面對準,且該等第二奈米線通 道側壁相對於該結晶面錯位。 5·如請求们或請求項2所述之方法,其中該等第—及第 二奈米線通道側壁均相對於該結晶面錯位。 6.如請求項1或請求項 ^ 卞2所述乙万沄其中該半導體材料 之該位移之步驟包含退火。 7.如請求項1或請求 步驟:將該等奈米 項2所述之方法,其進一 線通道再成形為奈米線。 步包含以下 步包含以下步驟:環繞 如請求項7所述之方法,其進一 16 201209930 該等奈米線中之每一者形成各個閘極。 . 9.如請求項8所述之方法,其中該辇胡〜A τ邊寺閘極各包含一介電 質、一薄閘極導體及摻雜導電材料。 1 0.如請求項8所 …丨…丨'咏分目卉有各個 驅動電流及/或閾電壓,該等驅動電流及/或閣電壓㈣ 該等第一及第二奈米線之該等厚度之間的該等差異而 同。 其中該形成之步驟 π .如請求項1或請求項2所述之方法, 包含一圖案化處理。 12.如請求項!所述之方法’其中第一奈米線通道側壁以相 對於該半導體之一結晶面之一第一對準度特徵化,且第 二奈米線通道側壁以相對於該結晶面之一第二對準度特 徵化,該第二對準度不同於該第一對準度。 1 3 · —種晶圓,其包含: 一基板; 一埋藏氧化物(BOX)層,其安置於該基板上;以及 一絕緣體上覆矽(SOI)結構,其安置在該BOX層上 於第一及第二區域處,在各區域處之該s〇I結構具有經 由其t形成之各個奈米線通道連接之各個S 〇1襯墊對, 17 201209930 處於該等區域中之—者之該等SOI襯墊及該等奈米 線通道較處於該等區域中之另一者之該等SOI襯墊及該 等奈米線通道相對於該SOI之{110}面更為錯位。 i 4.如請求項13所述之晶圓,其中該等錯位奈米線通道之 一輪廓涵蓋可由其形成之一再成形奈米線。 1 5 ·如呀求項13所述之晶圓’其中該等奈米線通道分別在 該等第〜及第二區域中之各者處彼此平行。 18201209930 VII. Patent Application Range: 1 · A method for modifying a wafer having a semiconductor disposed on an insulator, the method comprising the steps of: forming a semiconductor connected at each end to the first and second wafer regions The first and second nanowire channels of the liner, and the sidewalls of the second nanowire channel are misaligned to a greater extent than the crystalline side of the first nanowire channel; and The first and second nanowire channels of the Xuanzang displace the semiconductor material toward an alignment condition between the sidewall and the crystal plane such that the thickness difference between the first and second nanowire channels after the displacement Reflecting the larger misalignment of the sidewalls of the second nanowire channels. 2. A method of modifying a wafer having a semiconductor disposed on an insulator, the method comprising the steps of: forming a semiconductor profile connected by a nanowire channel in a first region of the wafer The nanowire channel has its major axis oriented along the {110} crystal planes of the semiconductor, and a sidewall substantially parallel to one of the {11 0 } faces of the semiconductor; Forming, in a second region, a semiconductor profile connected by a nanowire vial to the long axis of the nanochannel channel having an angle with respect to the {110} crystal faces of the semiconductor, and also relative to the The {11 〇} faces of the semiconductor are angled sidewalls; and the nanowire channels of the second region are reoriented to diffuse the semi-201209930 conductor material from the nanowire channels to the lining Forming a sidewall parallel to the {1 1 〇} faces of the semiconductor such that the nanowire channels in the second region are thinned compared to the nanowire channels in the first region . 3. The method of claim 1 or claim 2, wherein the step of forming comprises the steps of: forming the nanowire channels of the first region parallel to each other, and forming the second regions parallel to each other These nanowire channels. 4. The method of claim 1 or claim 2, wherein the first nanowire channel sidewalls are aligned with respect to the crystal face and the second nanowire channel sidewalls are misaligned relative to the crystal face. 5. The method of claim 2, wherein the sidewalls of the first and second nanowire channels are offset relative to the crystal plane. 6. The step of the displacement of the semiconductor material, as recited in claim 1 or claim ^2, comprises annealing. 7. The claim 1 or the request step: the method of the above item 2, which is reshaped into a nanowire in a line channel. The step includes the following steps: Surrounding as described in claim 7, which proceeds to a 16 201209930 each of the nanowires forms a respective gate. 9. The method of claim 8, wherein the gates of the 辇胡~A τ bian temple each comprise a dielectric material, a thin gate conductor, and a doped conductive material. 1 0. If the request item 8 is ... 丨 丨 咏 咏 卉 卉 卉 卉 卉 卉 卉 卉 , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , These differences between thicknesses are the same. The step of forming π. The method of claim 1 or claim 2 includes a patterning process. 12. As requested! The method 'where the sidewall of the first nanowire channel is characterized by a first alignment with respect to one of the crystal faces of the semiconductor, and the sidewall of the second nanowire channel is second with respect to one of the crystal faces The alignment is characterized by a second alignment that is different from the first alignment. 1 3 - a wafer comprising: a substrate; a buried oxide (BOX) layer disposed on the substrate; and an insulator overlying (SOI) structure disposed on the BOX layer At the first and second regions, the s〇I structure at each region has respective S 〇 1 pad pairs connected via respective nanowire channels formed by t, 17 201209930 being in the regions The SOI pads and the other nanowire channels are more misaligned relative to the {110} plane of the SOI than the other of the SOI pads in the other regions. The wafer of claim 13 wherein a contour of the misaligned nanowire channels encompasses one of the reshaped nanowires from which it can be formed. 1 5 - The wafer of claim 13 wherein the nanowire channels are parallel to each other in each of the first and second regions. 18
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